US10217532B2 - Systems and methods for merging and compressing compact tori - Google Patents

Systems and methods for merging and compressing compact tori Download PDF

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US10217532B2
US10217532B2 US15/483,984 US201715483984A US10217532B2 US 10217532 B2 US10217532 B2 US 10217532B2 US 201715483984 A US201715483984 A US 201715483984A US 10217532 B2 US10217532 B2 US 10217532B2
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acceleration
formation
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Michl W. Binderbauer
Vitaly Bystritskii
Toshiki Tajima
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TAE Technologies Inc
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    • G—PHYSICS
    • G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
    • G21B—FUSION REACTORS
    • G21B1/00—Thermonuclear fusion reactors
    • G21B1/03—Thermonuclear fusion reactors with inertial plasma confinement
    • G—PHYSICS
    • G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
    • G21B—FUSION REACTORS
    • G21B1/00—Thermonuclear fusion reactors
    • G21B1/05—Thermonuclear fusion reactors with magnetic or electric plasma confinement
    • G21B1/052—Thermonuclear fusion reactors with magnetic or electric plasma confinement reversed field configuration
    • G—PHYSICS
    • G21—NUCLEAR PHYSICS; NUCLEAR ENGINEERING
    • G21B—FUSION REACTORS
    • G21B3/00—Low temperature nuclear fusion reactors, e.g. alleged cold fusion reactors
    • G21B3/006—Fusion by impact, e.g. cluster/beam interaction, ion beam collisions, impact on a target
    • H—ELECTRICITY
    • H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
    • H05H—PLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
    • H05H1/00—Generating plasma; Handling plasma
    • H05H1/54—Plasma accelerators
    • H—ELECTRICITY
    • H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
    • H05H—PLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
    • H05H1/00—Generating plasma; Handling plasma
    • H05H1/02—Arrangements for confining plasma by electric or magnetic fields; Arrangements for heating plasma
    • H05H1/16—Arrangements for confining plasma by electric or magnetic fields; Arrangements for heating plasma using externally-applied electric and magnetic fields
    • Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E30/00—Energy generation of nuclear origin
    • Y02E30/10—Nuclear fusion reactors
    • Y02E30/122—

Definitions

  • the embodiments described herein relate generally to pulsed plasma systems and, more particularly, to systems and methods that facilitate merging and compressing compact tori with superior stability as well as significantly reduced losses and increased efficiency.
  • the Field Reversed Configuration belongs to the class of magnetic plasma confinement topologies known as compact toroids. It exhibits predominantly poloidal magnetic fields and possesses zero or small self-generated toroidal fields (see M. Tuszewski, Nucl. Fusion 28, 2033 (1988)).
  • the attractions of such a configuration are its simple geometry for ease of construction and maintenance, a natural unrestricted divertor for facilitating energy extraction and ash removal, and very high average (or external) ⁇ ( ⁇ is the ratio of the average plasma pressure to the average magnetic field pressure inside the FRC), i.e., high power density.
  • the ⁇ metric is also a very good measure of magnetic efficiency.
  • a high average ⁇ value e.g. close to 1, represents efficient use of the deployed magnetic energy and is henceforth essential for the most economic operation.
  • High average ⁇ is also critically enabling the use of aneutronic fuels such as D-He 3 and p-B 11 .
  • the traditional method of forming an FRC uses the field-reversed ⁇ -pinch technology, producing hot, high-density plasmas (see A. L. Hoffman and J. T. Slough, Nucl. Fusion 33, 27 (1993)).
  • a variation on this is the translation-trapping method in which the plasma created in a theta-pinch “source” is more-or-less immediately ejected out of the formation region and into a confinement chamber.
  • the translating plasmoid is then trapped between two strong mirrors at the ends of the confinement chamber (see, for instance, H. Himura, S. Okada, S. Sugimoto, and S. Goto, Phys. Plasmas 2, 191 (1995)).
  • FRCs have proved to be extremely robust, resilient to dynamic formation, translation, and violent capture events. Moreover, they show a tendency to assume a preferred plasma state (see e.g. H. Y. Guo, A. L. Hoffman, K. E. Miller, and L. C. Steinhauer, Phys. Rev. Lett. 92, 245001 (2004)).
  • FRCs consist of a torus of closed field lines inside a separatrix, and of an annular edge layer on the open field lines just outside the separatrix. The edge layer coalesces into jets beyond the FRC length, providing a natural divertor.
  • the FRC topology coincides with that of a Field-Reversed-Mirror plasma.
  • the FRC plasma can have an internal ⁇ of about 10.
  • the inherent low internal magnetic field provides for a certain indigenous kinetic particle population, i.e. particles with large larmor radii, comparable to the FRC minor radius. It is these strong kinetic effects that appear to at least partially contribute to the gross stability of past and present FRCs, such as those produced in the recent collision-merging experiments.
  • the collision-merging technique proposed long ago (see e.g. D. R. Wells, Phys. Fluids 9, 1010 (1966)) has been significantly developed further: two separate theta-pinches at opposite ends of a confinement chamber simultaneously generate two plasmoids (e.g., two compact tori) and accelerate the plasmoids toward each other at high speed; they then collide at the center of the confinement chamber and merge to form a compound FRC.
  • the conventional collision-merging method was shown to produce stable, long-lived, high-flux, high temperature FRCs (see e.g. M. Binderbauer, H. Y. Guo, M.
  • the precursor system described in Bystritskii featured simultaneous compression and acceleration of compact tori within the same stage by using active fast magnetic coils. Five such stages were deployed on either side of a central compression chamber before magnetically compressing the merged compact tori. While the precursor experiment achieved respectable performance, it exhibited the following deficiencies: (1) Simultaneous compression and acceleration led to inefficient use of driver energy deployed for magnetic compression due to a timing mismatch; (2) Temperature and density decreased as plasma expanded during transit between sections; (3) Abrupt transitions between adjacent sections led to large losses due to plasma-wall contact and generation of shockwaves.
  • pulsed fusion concepts in the medium density regime will have to address adequate transport timescales, efficient drivers, rep-rate capability and appropriate final target conditions. While the precursor system has successfully achieved stable single discharges at encouraging target conditions, the collective losses between formation and final target parameters (presently about 90% of the energy, flux, and particles) as well as the coupling efficiency between driver and plasma (at present around 10-15%) need to be substantially improved.
  • the present embodiments provided herein are directed to systems and methods that facilitate merging and compressing compact tori with superior stability as well as a significant reduction of translation and compression losses and an increase in coupling efficiency between drivers and plasma.
  • Such systems and methods provide a pathway to a whole variety of applications including compact neutron sources (for medical isotope production, nuclear waste remediation, materials research, neutron radiography and tomography), compact photon sources (for chemical production and processing), mass separation and enrichment systems, and reactor cores for fusion for the future generation of energy and for fusion propulsion systems.
  • the systems and methods described herein are based on the application of successive, axially symmetric acceleration and adiabatic compression stages to accelerate and heat two compact tori towards each other and ultimately collide and fast magnetically compress the compact tori within a central compression chamber.
  • a system for merging and compressing compact tori comprises a staged symmetric sequence of compact tori formation, axial acceleration by fast active magnetic coils, passive adiabatic compression by way of a conically constricting flux conserver, and ultimately merging of the compact tori and final fast magnetic compression in a central compression chamber.
  • the intermediate steps of sufficient axial acceleration followed by adiabatic compression can be repeated multiple times to achieve adequate target conditions before merging and final compression. In this way, a reactor can be realized by adding further sections to the system.
  • the formation and accelerations stages or sections and the central compression chamber are preferably cylindrically shaped with walls formed of non-conducting or insulating material such as, e.g., a ceramic.
  • the compressions stages or sections are preferably trunco-conically shaped with walls formed from conducting material such as, e.g., a metal.
  • the formation sections, the acceleration sections, and the compression chamber include modular pulsed power systems that drive fast active magnetic coils.
  • the slow or DC magnetic coil systems located throughout and along the axis of the system provide an axial magnetic guide field to center the compact tori appropriately as it translates through the section toward the mid-plane of the central compression chamber.
  • the systems and methods described herein deploy FRCs, amongst the highest beta plasmas known in magnetic confinement, to provide the starting configuration. Further passive and active compression builds on this highly efficient magnetic topology.
  • the process of using axial acceleration via active fast magnet sections followed by adiabatic compression in simple flux conserving conic sections provides for the most efficient transfer of energy with the least complex pulsed power circuitry.
  • these basic building blocks can be sequenced to take additional advantage of the inherently favorable compressional scaling, i.e. ⁇ p ⁇ R 4 .
  • system is configured to deploy spheromaks instead of FRC starter plasmas.
  • the system comprises a staged asymmetric sequence from a single side of the central compression chamber comprising compact tori formation, axial acceleration by fast active magnetic coils, passive adiabatic compression by way of a conically constricting flux conserver, and ultimately merging of the compact tori and final fast magnetic compression in the central compression chamber.
  • asymmetric system would include a mirror or bounce cone positioned adjacent the other side of the central compression.
  • the system comprises a thin cylindrical shell or liner comprised of conductive material such as, e.g., a metal, for fast liner compression within the central compression chamber.
  • conductive material such as, e.g., a metal
  • FIG. 1 illustrates a basic layout of a system for forming, accelerating, adiabatically compressing, merging and finally magnetically compressing compact tori.
  • FIG. 2 illustrates a schematic of the components of a pulsed power system for the formation and acceleration sections.
  • FIG. 3 illustrates an isometric view of an individual pulsed power formation and acceleration skid.
  • FIG. 4 illustrates an isometric view of a formation and acceleration tube assembly.
  • FIG. 5 illustrates a basic layout of an alternate embodiment of an asymmetric system for forming, accelerating, adiabatically compressing, merging and finally magnetically compressing compact tori.
  • FIG. 6 illustrates a detailed view of the system shown in FIG. 1 modified to include a shell or liner positioned within the central compression chamber for fast liner compression within the central compression chamber.
  • the present embodiments provided herein are directed to systems and methods that facilitate merging and compressing compact tori with superior stability as well as a significant reduction of translation and compression losses and an increase in coupling efficiency between drivers and plasma.
  • Such systems and methods provide a pathway to a whole variety of applications including compact neutron sources (for medical isotope production, nuclear waste remediation, materials research, neutron radiography and tomography), compact photon sources (for chemical production and processing), mass separation and enrichment systems, and reactor cores for fusion for the future generation of energy and for fusion propulsion systems.
  • FIG. 1 illustrates the basic layout of a system 10 for forming, accelerating, adiabatically compressing, merging and finally magnetically compressing the compact tori.
  • the system comprises a staged symmetric sequence of compact tori formation in formation sections 12 N and 12 S, axial acceleration through sections 12 N, 12 S, 16 N and 16 S by fast active magnetic coils 32 N, 32 S, 36 N and 36 S, passive adiabatic compression by way of a conically constricting flux conserver in sections 14 N, 14 S, 18 N and 18 S, and ultimately merging of the compact tori and final fast magnetic compression in a central compression chamber 20 by fast active magnetic coils 40 .
  • the intermediate steps of sufficient axial acceleration followed by adiabatic compression can be repeated multiple times to achieve adequate target conditions before merging and final compression. In this way, a reactor can be realized by adding further sections to the depicted system.
  • the formation and accelerations stages or sections 12 N, 12 S, 16 N and 16 S and the central compression chamber 20 are preferably cylindrically shaped with walls formed of non-conducting or insulating material such as, e.g., a ceramic.
  • the compressions stages or sections 14 N, 14 S, 18 N and 18 S are preferably trunco-conically shaped with walls formed from conducting material such as, e.g., a metal.
  • the formation sections 12 N and 12 S, the acceleration sections 16 N and 16 S, and the compression chamber 20 include modular pulsed power systems that drive fast active magnetic coils 32 N, 32 S, 36 N, 36 S and 40 .
  • the slow passive magnetic coil systems 30 located throughout and along the axis of the system provide an axial magnetic guide field to center the compact tori appropriately.
  • the systems and methods described herein deploy FRCs, amongst the highest beta plasmas known in magnetic confinement, to provide the starting configuration. Further passive and active compression builds on this highly efficient magnetic topology.
  • the process of using axial acceleration via active fast magnet sections followed by adiabatic compression in simple flux conserving conic sections provides for the most efficient transfer of energy with the least complex pulsed power circuitry.
  • these basic building blocks can be sequenced to take additional advantage of the inherently favorable compressional scaling, i.e. ⁇ p ⁇ R 4 .
  • system is configured to deploy spheromaks instead of FRC starter plasmas.
  • the system comprises a staged asymmetric sequence from a single side of the central compression chamber comprising compact tori formation, axial acceleration by fast active magnetic coils, passive adiabatic compression by way of a conically constricting flux conserver, and ultimately merging of the compact tori and final fast magnetic compression in the central compression chamber.
  • asymmetric system would include a mirror or bounce cone.
  • the system comprising a thin cylindrical shell or liner comprised of conductive material such as, e.g., a metal, for fast liner compression within the central compression chamber.
  • conductive material such as, e.g., a metal
  • a system 10 for merging and compressing compact tori plasma includes a central compression chamber 20 and a pair of north and south diametrically opposed compact tori formation sections 12 N and 12 S.
  • the first and second formation sections 12 N and 12 S include a modularized formation and acceleration systems 120 (discuss below in detail with regard to see FIGS. 2-4 ) for generating first and second compact plasma tori and axially accelerating and translating the compact tori towards a mid-plane of the compression chamber 20 .
  • the system 10 further includes a first pair of north and south diametrically opposed compression sections 14 N and 14 S coupled on a first end to an exit end of the north and south formation sections 12 N and 12 S.
  • the north and south compression sections 14 N and 14 S being configured to adiabatically compress the compact tori as the compact tori traverse the north and south compression sections 14 N and 14 S towards the mid-plane of the compression chamber 20 .
  • the system 10 further includes a pair of north and south diametrically opposed acceleration sections 16 N and 16 S coupled on a first end to a second end of the first pair of north and south compression sections 14 N and 14 S.
  • the north and south acceleration section 16 N and 16 S include modularized acceleration systems (discussed below with regard to FIGS. 2-4 ) for axially accelerating and translating the compact tori towards the mid-plane of the compression chamber 20 .
  • the system 10 further includes a second pair of north and south diametrically opposed compression sections 18 N and 18 S coupled on a first end to a second end of the north and south acceleration sections 16 N and 16 S and on a second end to first and second diametrically opposed ends of the compression chamber, the second pair of north and south compression sections 18 N and 18 S being configured to adiabatically compress the compact tori as the compact tori traverse the second pair of north and south compression sections 18 N and 18 S towards the mid-plane of the compression chamber 20 .
  • the compression chamber includes a modularized compression systems configured to magnetically compress the compact tori upon collision and merger thereof.
  • the north and south acceleration sections 16 N and 16 S and the compression chamber 20 are cylindrically shaped.
  • the diameter of the north and south acceleration sections 16 N and 16 S is smaller than the diameter of the north and south formation sections 12 N and 12 S, while the diameter of the compression chamber 20 is than the diameter of the north and south acceleration sections 16 N and 16 S.
  • the first and second pairs of north and south compression sections 14 N, 14 S, 18 N and 18 S are truncated conically shaped with their diameter being larger on a first end than on a second end enabling a transition in the overall diameter of the system 10 from the formation sections 12 N and 12 S to the acceleration sections 16 N and 16 S to the compression chamber 20 .
  • the north and south formation sections 12 N and 12 S, the first pair of north and south compression sections 14 N and 14 S, the north and south acceleration sections 16 N and 16 S, and the second pair of north and south compression sections 18 N and 18 S are axially symmetric.
  • first and second sets of a plurality of active magnetic coils 32 N and 32 are disposed about and axially along the north and south formation sections 12 N and 12 S
  • third and fourth sets of a plurality of active magnetic coils 36 N and 36 S are disposed about and axially along the north and south acceleration sections 16 N and 16 S
  • a fifth set of a plurality of active magnetic coils 40 are disposed about and axially along the compression chamber 20 .
  • the compression sections 14 N, 14 S, 18 N and 18 S are preferably formed from conducting material such as, e.g., a metal, while the central compression chamber 20 and the formation and acceleration sections are 12 N, 12 S, 16 N and 16 S are preferably formed from non-conducting or insulating material such as, e.g., a ceramic.
  • a plurality of DC magnetic coils 30 are disposed about and axially along the central compression chamber 20 and the formation, compression and acceleration sections 12 N, 12 S, 14 N, 14 S, 16 N, 16 S, 18 N and 18 S to form a bias or DC guide field within and extending axially through the central compression chamber and the formation, compression and acceleration sections.
  • Triggering control and switch systems 120 are configured to enable a staged symmetric sequence of compact tori formation by active magnetic coils 32 N and 32 S in the north and south formation sections 12 N and 12 S, axial acceleration by active magnetic coils 36 N and 36 S in the north and south acceleration sections 16 N and 16 S, and compression by active magnetic coils 40 in the compression chamber 20 .
  • the triggering control and switch systems 120 are configured to synchronize compact tori formation and acceleration in the north and south formation sections 12 N and 12 S, compact tori acceleration in the north and south acceleration sections 16 N and 16 S, and compact tori merge and compression in the compression chamber 20 .
  • FIGS. 2-4 there is individual pulsed power system 120 corresponding to and powering individual ones of the first, second, third, fourth and fifth sets of the plurality of active magnets 32 N, 32 S, 36 N, 36 S and 40 of the formation sections 12 N and 12 S, the acceleration sections 16 N and 16 S, and the compression chamber 20 .
  • the pulse power system 120 operates on a modified theta-pinch principle to form the compact tori.
  • FIGS. 2 through 4 illustrate the main building blocks and arrangement of the pulsed power systems 120 .
  • Each skid 122 is composed of capacitors 121 , inductors 123 , fast high current switches 125 and associated trigger 124 and dump circuitry 126 . Coordinated operation of these components is achieved via a state-of-the-art trigger and control system 124 and 126 that allows synchronized timing between the pulsed power systems 120 on each of the formation sections 12 N and 12 S, the acceleration sections 16 N and 16 S, and compression chamber 20 , and minimizes switching jitter to tens of nanoseconds.
  • a DC guide field is generated by the passive coils 30 within and axially extending through the compression chamber 20 , the formation sections 12 N and 12 S, the acceleration sections 16 N and 16 S, and the compression sections 14 N, 14 S, 18 N and 18 S.
  • Compact tori are then formed and accelerated in a staged symmetric sequence within the formation sections 12 N and 12 S and the acceleration sections 16 N and 16 S towards a mid-plane of the central chamber 20 , passively adiabatically compressed within the compression sections 14 N, 14 S, 18 N and 18 S, and merged and magnetically compressed within the central chamber 20 .
  • the compact tori are formed and accelerated by powering active magnetic coils 32 N and 32 S extending about and axially along the formation sections 12 N and 12 S, further accelerated by powering active magnetic coils 35 N and 36 S extending about and axially along the acceleration sections 16 N and 16 S, and compressed by powering active magnetic coils 40 extending about and axially along the compression chamber 20 .
  • the steps of forming, accelerating and compressing the compact tori further comprises synchronously firing diametrically opposed pairs of active magnetic coils 32 N and 32 S, and 36 N and 36 S positioned about and along the formation 12 N and 12 S and acceleration sections 16 N and 16 S, and a set of active magnetic coils 40 positioned about and along the compression chamber 20 .
  • the compact tori are compressed as the compact tori translate through the conically constricting flux conservers of the compression stages 14 N, 14 S, 18 N and 18 S.
  • the system 100 comprises a staged asymmetric sequence from a single side of the central compression chamber 20 .
  • the system 100 includes a single compact toroid formation section 12 S, a first compression section 14 S coupled on a first end to an exit end of the formation section 12 S, an acceleration section 16 N coupled on a first end to a second end of the compression section 14 S, a second compression section 18 S coupled on a first end to a second end of the acceleration section 16 S and on a second end to a first end of the compression chamber 20 .
  • a mirror or bounce cone 50 is positioned adjacent the other end of the central compression 20 .
  • a first compact toroid is formed and accelerated in a staged sequence within the formation section 12 S and then accelerated in one or more acceleration stages 16 S towards a mid-plane of the central chamber 20 to collide and merge with a second compact toroid.
  • the first compact toroid is passively adiabatically compressed within one or more compression stages 14 S and 18 S, and then magnetically compressed as a merged compact toroid with the second compact toroid within the central chamber 20 .
  • the second compact toroid in formed and accelerated in a staged sequence within the formation section 12 S and the one or more acceleration stages 16 S towards a mid-plane of the central chamber 20 , passively adiabatically compressed within the one or more compression stages, and then biased back toward the mid-plane of the central chamber 20 as it passes through the central chamber 20 with a mirror or bounce cone 50 positioned adjacent an end of the central chamber 20 .
  • FIG. 6 an alternative embodiment of a system 200 for merging and compressing compact tori plasma is illustrated in a partial detail view showing the compression chamber 20 with diametrically opposed compression section 18 N and 18 S coupled to opposing sides of the chamber 20 .
  • the system 200 further comprise a cylindrical shell or liner 60 positioned within the central compression chamber 20 for fast liner compression.

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